DNP for polarizing liquid 3 He DNP for polarizing liquid 3 He Hideaki Uematsu Department of Physics Yamagata University.

Slides:



Advertisements
Similar presentations
Patricia Aguar Bartolomé Institut für Kernphysik, Universität Mainz PSTP 2013 Workshop, Charlottesville 11th September 2013.
Advertisements

Electron Spin Resonance (ESR) Spectroscopy
CI 3.2 The size of ions Ions in solution Attractions to other ions and to water molecules depend on: Charge on the ion Size of the ion.
Resonant Transition = “spin flip” of electron Allowed transitions:  M s = + 1 = 9.6 GHz (X-band microwave) Ex) One unpaired electron: E  E = h M s =
An Introduction to Parahydrogen Projects in the Pines Lab David Trease Special Topics... March Chip Crawford.
Radical Recombination Kinetics. Objectives To synthesize a dimer, which upon irradiation, undergoes dissociation to a radical Determine the order and.
Magnetic Field (B) A photon generates both an electric and a magnetic field A current passing through a wire also generates both an electric and a magnetic.
Structure Determination by NMR CHY 431 Biological Chemistry Karl D. Bishop, Ph.D. Lecture 1 - Introduction to NMR Lecture 2 - 2D NMR, resonance assignments.
NMR Spectroscopy Part II. Signals of NMR. Free Induction Decay (FID) FID represents the time-domain response of the spin system following application.
Rinat Ofer Supervisor: Amit Keren. Outline Motivation. Magnetic resonance for spin 3/2 nuclei. The YBCO compound. Three experimental methods and their.
Introduction to Water. Created by Dr. Michael Pidwirny, Department of Geography, Okanagan University College, BC, CA evaporation Soil and Water.
Noise near peak field is increased Peak width narrow Peak is symmetric Purpose: Resonate nuclei to prevent polarization. Matching the resonant frequencies.
Coherent Manipulation and Decoherence of S=10 Fe8 Single- Molecule Magnets Susumu Takahashi Physics Department University of California Santa Barbara S.
Optically Pumping Nuclear Magnetic Spin M.R.Ross, D.Morris, P.H. Bucksbaum, T. Chupp Physics Department, University of Michigan J. Taylor, N. Gershenfeld.
Determination Of Magnetic Moments In Metal-Metal Bonded Complexes
SPIN 2004 Oct. 14, 2004 W. Kim, S.S. Stepanyan, S. Woo, M. Rasulbaev, S. Jin (Kyungpook National University) S. Korea Polarization Measurements of the.
ELECTRON SPIN RESONANCE SPECTROCOPY
Tools of the Trade 1- Atomic resolution: X-ray crystallography 2- NMR spectroscopy 3- de novo Modeling and structure determination, Homology modeling 4-
Electron Spin Resonance Spectroscopy
1 Femtosecond Time and Angle-Resolved Photoelectron Spectroscopy of Aqueous Solutions Toshinori Suzuki Kyoto University photoelectron.
 PART Requirements for Spectroscopic Techniques for Polymers 1. High resolution 2. High sensitivity (>1%) 3. High selectivity between molecular.
Physical Chemistry 2 nd Edition Thomas Engel, Philip Reid Chapter 28 Nuclear Magnetic Resonance Spectroscopy.
What is the chemical formula for water? Draw the structure of water. Write down all the types of bonding that you know of.
Chapter 11. Liquids, Solids & Forces of Attraction CHE 124 General Chemistry II Dr. Jerome K. Williams, PhD Saint Leo University.
Magnetic Resonance Contributions to Other Sciences Norman F. Ramsey Harvard University Principles of Magnetic Resonance First experiments Extensions to.
DHB, nEDM Collab. Mtg, 15/16 Apr 04 UIUC Test System (Beck, Chandler, Hertzog, Kammel, Newman, Peng, Sharp, Williamson, Yoder; Blackburn, Kenyon, Thorsland)
Laser-microwave double resonance method in superfluid helium for the measurement of nuclear moments Takeshi Furukawa Department of Physics, Graduate School.
Chapter 3 Nuclear Magnetic Resonance Spectroscopy Many atomic nuclei have the property of nuclear spin. When placed between the poles of a magnet, the.
Dark Matter Search with Direction sensitive Scintillator Ⅱ Department of Physics, School of Science The University of Tokyo Y. Shimizu, M. Minowa, Y. Inoue.
Key Vocabulary Matter and changes Mixtures Atoms Periodic Table PotpourriAcids and Bases States of Matter
Chemistry Chapter Two. What is Chemistry? Chemistry- the study of matter, atoms and chemical reactions –Why? to understand how our cells are held together.
NMR spectroscopy in solids: A comparison to NMR spectroscopy in liquids Mojca Rangus Mentor: Prof. Dr. Janez Seliger Comentor: Dr. Gregor Mali.
Intro to NMR for CHEM 645 we also visited the website: The Basics of NMR by Joseph P. Hornak, Ph.D. The Basics of NMR.
An attempt toward dynamic nuclear polarization for liquid 3 He 1. Motivation of the study 2 . Polarizing 3 He in dense form 3. DNP for liquid He3 3 . Doping.
Biology Properties of Water. Matter consists of chemical elements in pure form and in combinations called compounds Organisms are composed of matter Matter.
Naoki Komatsu 1, Marc Dubois 2, Katia Guérin 2, André Hamwi 2, Jérôme Giraudet 3, Françis Masin 3 1 Shiga University of Medical Science (SUMS), Department.
Bradford Michael Mess, John J. Banisaukas III, and Lon B. Knight, Jr.
Motivation Polarized 3 He gas target Solenoid design and test 3 He feasibility test Summary and outlook Johannes Gutenberg-Universit ä t Mainz Institut.
Ultrahigh precision observation of nuclear spin precession and application to EDM measurement T. Inoue, T. Furukawa, H. Hayashi, M. Tsuchiya, T. Nanao,
HD target. HD target overview Characteristics of polarized HD target Polarization Method HD target is polarized by the static method using “brute force”
Nuclear Magnetic Resonance
EPR Study of Vanadyl Complexes
Polarized Proton Solid Target for RI beam experiments M. Hatano University of Tokyo H. Sakai University of Tokyo T. Uesaka CNS, University of Tokyo S.
ELECTRON AND PHONON TRANSPORT The Hall Effect General Classification of Solids Crystal Structures Electron band Structures Phonon Dispersion and Scattering.
Low–field NMR (or MRI) Images of Laser polarized Noble Gas.
1 XI International Workshop PST05 Tokyo, Japan, November 14-17, 2005 The Sb and HIO 3 Aligned Nuclear Targets for Investigation of Time Reversal Invariance.
Ch. 11 States of matter. States of Matter Solid Definite volume Definite shape Liquid Definite volume Indefinite shape (conforms to container) Gas Indefinite.
Spin Dynamics of Superfluid 3 He in Aerogel Osamu Ishikawa Osaka City University.
Matter anything that has mass and takes up space.
Analysis of the Ammonia Target Polarization Kangkang L. Kovacs, Physics Department, University of Virginia, Charlottesville, VA
9 th Crystal Ball Meeting Basel October Andreas Thomas Transversely Polarized Target 1.-Possible Physics Experiments 2.-Frozen Spin Target 3.-Technical.
Unit 6: Chemical Bonding Refer to Ch. 8 & 9 for supplemental reading.
Laser-Driven H/D Target at MIT-Bates Ben Clasie Massachusetts Institute of Technology Ben Clasie, Chris Crawford, Dipangkar Dutta, Haiyan Gao, Jason Seely.
Recent Developments in Polarized Solid Targets H. Dutz, S. Goertz Physics Institute, University Bonn J. Heckmann, C. Hess, W. Meyer, E. Radke, G. Reicherz.
* Ask as many questions as you can on the topic of state of matter:
1 Possibility to obtain a polarized hydrogen molecular target Dmitriy Toporkov Budker Institute of Nuclear Physics Novosibirsk, Russia XIV International.
J. Kohlbrecher, Polarized Solid Targets, Honnef 2003 Dynamics Of Nuclear Spin Polarization J. Kohlbrecher Paul Scherrer Institute CH-5232 Villigen Switzerland.
Study of T 1 relaxation time A proposal to test T 1 using a dilution fridge and SQUID NMA at Royal Hollow University,London.
DNP for polarizing liquid 3 He DNP for polarizing liquid 3 He Akira Tanaka Department of Physics For Yamagata University PT group.
Characteristic Physical Properties. Characteristic physical properties are properties that are unique to a substance and can be used to identify it. For.
First Principle Calculation of Nuclear Magnetic Resonance (NMR) chemical shift Kanchan Sonkar Center of Biomedical Magnetic Resonance SGPGIMS-Campus, Lucknow,
17th Crystal Ball Meeting
Ch Solutions. Sec. 1 – How Solutions Form Solution = homogeneous mixture mixed at the molecular level; may be liquids, gases, or solids(alloy) Solute.
Powerpoint Templates Page 1 Powerpoint Templates Electronic Spectroscopy NMR.
DNP for polarizing liquid 3 He DNP for polarizing liquid 3 He Hideaki Uematsu Department of Physics For Yamagata University PT group.
Double spin asymmetry measurement from SANE-HMS data at Jefferson Lab Hoyoung Kang For SANE collaboration Seoul National University DIS /04/23.
Nuclear magnetic resonance Spectroscopy Basic Concept.
Solid-State NMR signal enhancement via DNP from endogenous flavin.
Strong Coupling of a Spin Ensemble to a Superconducting Resonator
 .
Presentation transcript:

DNP for polarizing liquid 3 He DNP for polarizing liquid 3 He Hideaki Uematsu Department of Physics Yamagata University

Member(2006) T.Shishido, T.Iwata, S.Kato, T.Michigami, S.Ohizumi, Y.Tajima, A.Tanaka, K.Toyama, H.Uematsu, and H.Y.Yoshida Department of Physics, Yamagata University, Yamagata N.Kuriyama Department of Material and Biological Chemistry, Yamagata University, Yamagata

Background of the study Polarized 3 He targets have been used in various scattering experiments Polarized 3 He targets have been used in various scattering experiments > In 3 He only neutron is polarized > In 3 He only neutron is polarized > A good target for the study of neutron characteristics > A good target for the study of neutron characteristics > Studied only in gas targets > Studied only in gas targets Advantages of polarizing liquid 3 He Advantages of polarizing liquid 3 He >Density ⇒ := 1 : 662 >Density ⇒ gas:liquid= 1 : 662 >Its fluidity may allow to make a polarized target with circulating polarized liquid 3 He >Its fluidity may allow to make a polarized target with circulating polarized liquid 3 He >Could be applied in many other fields >Could be applied in many other fields (e.g. medical use, material science, etc.) (e.g. medical use, material science, etc.)

How to obtain polarized liquid 3 He 1. From polarized solid 3 He >Polarized liquid is obtained by quickly melting polarized solid >Polarized liquid is obtained by quickly melting polarized solid >55% polarization obtained in solid at 6.6T, 6mK, and 30bar, G.Bonfait et al. Phys.Rev.Lett. 53(1984)1092 >55% polarization obtained in solid at 6.6T, 6mK, and 30bar, G.Bonfait et al. Phys.Rev.Lett. 53(1984)1092 → required special equipments to make 3 He solid → required special equipments to make 3 He solid 2. Dynamic Nuclear Polarization (DNP) > spin-spin coupling between electron and nucleus > spin-spin coupling between electron and nucleus >Transferring polarization of electrons to neighboring nuclei >Transferring polarization of electrons to neighboring nuclei >Both positive and negative polarization available >Both positive and negative polarization available

US group applied DNP for polarizing liquid 3 He powdered sucrose charcoal powdered sucrose charcoal Polarization process: Polarization process: electron → 1 H → 3 He of TE signal amplitude 1.18 times of TE signal amplitude (T= 1.8 K, B= 182 G) Relaxation time Relaxation time T 1 = 1.02sec L.W.Engel et al. L.W.Engel et al. Phys. Rev. B 33, 2035 (1986) DNP Polarization transfer H↑H↑ e charcoal Liq. 3 He RF

fluorocarbon beads containing electronic paramagnetic centers fluorocarbon beads containing electronic paramagnetic centers Polarization process: Polarization process: electron → 19 F → 3 He a. Positive: of TE signal at a. Positive: twice of TE signal at T= 250 mK, B= 300 G b. Negative: not mentioned A.Schuhl et al. A.Schuhl et al. Phys. Rev. Lett. 54,1952 (1985) French group applied DNP for polarizing liquid 3 He DNP 3 He 19 F H TE 3 He Polarization transfer F↑F↑ e fluorocarbon Liq. 3 He RF

Our New DNP method for polarizing liquid 3 He Direct coupling between electron and 3 He Direct coupling between electron and 3 He Using unpaired electrons in free radical Using unpaired electrons in free radical Embedding free radicals into porous material Embedding free radicals into porous material Filling the porous material with liquid 3 He Filling the porous material with liquid 3 He Microwave irradiation Microwave irradiation  Free radical →  Free radical → TEMPO  Porous material →  Porous material → Zeolite

Zeolite and TEMPO NaY type zeolite (n=51) NaY type zeolite (n=51) Super Cage Max dia.: 13Å Window dia.: 7.4Å 4.7x10 19 super cages/g A super cage can store 80 3 He atoms TEMPO (2,2,6,6-tetramenthyl- piperidinyl-1-oxyle) TEMPO (2,2,6,6-tetramenthyl- piperidinyl-1-oxyle) Melting point: 36 º C Boiling point: 67 º C Molecule size: ~7Å sodalite cage double T6-ring Zeolite(Na n Al n Si (192-n) O 384 ·240H 2 O (n=48~76 ) HH CH 3 H3CH3C H3CH3C H H H H N O TEMPO 7Å7Å 7.4Å ESR signal of TEMPO in zeolite super cage

Embedding TEMPO to Zeolite Preparation : Desiccate zeolite at 500 ºC for 8 hours Preparation : Desiccate zeolite at 500 ºC for 8 hours 1. Dissolve TEMPO in n- pentane 2. Add zeolite powder to n- pentane solution 3. Stir n-pentane solution for 8 hours in a sealed vessel 4. Evaporate n-pentane in a vacuum container 500 ºC Zeolite

Embedding TEMPO to Zeolite TEMPO n-pentane Preparation : Desiccate zeolite at 500 ºC for 8 hours Preparation : Desiccate zeolite at 500 ºC for 8 hours 1. Dissolve TEMPO in n- pentane 2. Add zeolite powder to n- pentane solution 3. Stir n-pentane solution for 8 hours in a sealed vessel 4. Evaporate n-pentane in a vacuum container zeolite

Embedding TEMPO to Zeolite Preparation : Desiccate zeolite at 500 ºC for 8 hours Preparation : Desiccate zeolite at 500 ºC for 8 hours 1. Dissolve TEMPO in n- pentane 2. Add zeolite powder to n- pentane solution 3. Stir n-pentane solution for 8 hours in a sealed vessel 4. Evaporate n-pentane in a vacuum container

Embedding TEMPO to Zeolite Preparation : Desiccate zeolite at 500 ºC for 8 hours Preparation : Desiccate zeolite at 500 ºC for 8 hours 1. Dissolve TEMPO in n- pentane 2. Add zeolite powder to n- pentane solution 3. Stir n-pentane solution for 8 hours in a sealed vessel 4. Evaporate n-pentane in a vacuum container pump

Experimental setup  Experimental cell made of a PET tube and a VCR gas connector  Volume : 2.5cc (L=35mm, φ=9mm)  Experimental cell filled with zeolite tightly and quickly Experimental cell experimental chamber

Thermal equilibrium signal of 3 He T= 1.42 K, B ≒ 2.5 T 1.3×10 19 electron spins/cc T= 1.47 K, B ≒ 2.5 T Low spin density (with zeolite) 0.45×10 19 electron spins/cc T= 1.54 K, B ≒ 2.5 T High spin density (with zeolite)Bulk 3 He (without zeolite) Symmetric signal when 3 He in zeolite Symmetric signal when 3 He in zeolite Narrower width for low spin density Narrower width for low spin density Bulk 3 He signal shows asymmetric shape Bulk 3 He signal shows asymmetric shape

TE signals fitted with Lorentzian T= 1.42 K,B ≒ 2.5 T 1.3×10 19 spins/cc T= 1.47 K, B ≒ 2.5 T 0.45×10 19 spins/cc T= 1.54 K, B ≒ 2.5 T Extent: 44.4 ppm Bulk 3He(without zeolite) Center frequency of 3 He: Center frequency of 3 He: f c = 81.09MHz (at 2.5T) Extent: 202 ppm High spin density (with zeolite)Low spin density (with zeolite) FWHM ※ Extent=FWHM/f c

Relaxation time of liquid 3 He Fitting function S: area of the NMR signal Time development of NMR signal of liquid 3 He inside zeolite, spin density: T= 1.44 K, B= 2.5 T, spin density: 1.3×10 19 spin/cc Relaxation time: Relaxation time: T 1 = 330 sec. 3 He in zeolite with TEMPO

Positive enhancement by DNP TE signal T= 1.48 K, B ≒ 2.5 T max polarized signal B ≒ 2.5 T observed positive enhancement observed positive enhancement S/S TE = 2.34 spin density= (low concentration) spin density= 0.45×10 19 (low concentration)

Negative enhancement by DNP TE signal T= 1.53 K, B ≒ 2.5 T max polarized signal B ≒ 2.5 T observed negative enhancement S/S TE =-1.59 spin density= spin density= 0.45× polarized TE

Microwave frequency dependence fc: ESR center frequency of TEMPO(=70.22GHz) of TEMPO(=70.22GHz) spin density: spin density: 1.3×10 19, B ≒ 2.5T Frequency difference(250MHz) between max enhancement points is smaller than that expected from the calculated ESR line width( 340 MHz ※ ) ※ S.T.Gortez, et al. Nucl. Instrum. and Meth A526, 43 (2004) 250MHz 340MHz

Summary We observed the thermal equilibrium signals of liquid 3 He in zeolite. We observed the thermal equilibrium signals of liquid 3 He in zeolite. A narrow signal was observed with low electron spin density. A narrow signal was observed with low electron spin density. We measured relaxation time of 3 He in zeolite (a few minutes at 2.5T) We measured relaxation time of 3 He in zeolite (a few minutes at 2.5T) We obtained polarization enhancements for liquid 3 He in zeolite by DNP. We obtained polarization enhancements for liquid 3 He in zeolite by DNP.  The enhancements were larger than ever before (obtained by DNP).  They may be improved by tuning the conditions.

Thank you for listening

Zeolite and its character Mineral which has a micro-porous structure, high hydrophobicity, thermostability and mostly used as a catalyst, ion exchanger, absorber Mineral which has a micro-porous structure, high hydrophobicity, thermostability and mostly used as a catalyst, ion exchanger, absorber (Na n Al n Si (192-n) O 384 ·240H 2 O (n=48~76 ) (Na n Al n Si (192-n) O 384 ·240H 2 O (n=48~76 ) Used (HSZ-300serise)TOSOH corporation Used (HSZ-300serise)TOSOH corporation Cation type: Na Cation type: Na SiO 2 /Al 2 O 3 (mol/mol): 5.5 SiO 2 /Al 2 O 3 (mol/mol): 5.5 Na2O(wt%): 12.5 Na2O(wt%): 12.5 U.C.C. by ASTM :24.63 U.C.C. by ASTM :24.63 NH3-TPD(mmol/g): - NH3-TPD(mmol/g): - Surface Area(BET, m2/g): 700 Surface Area(BET, m2/g): 700 Crystal Size(μm): 0.3 Crystal Size(μm): 0.3 Mean Particle Size(μm): 6 Mean Particle Size(μm): 6

Zeolite’s atom atomspin Magnetic moment Abundance(%) 16 O O 5/ O Na 3/ Al 5/ Si Si 1/ Si

Decrease of TEMPO in Zeolite Spin density :7.5×10 18 spin/cc Room temperature

n-pentane C 5 H 12 C 5 H 12 melting point: -131ºC melting point: -131ºC boiling point: 36.07ºC boiling point: 36.07ºC →0.13% Density of liquid 3 He in 1g zeolite in 1g zeolite23.1mg